SUBROUTINE boundary_conds

!--------------------------------------------------------------------------------!
! This file is part of PALM.
!
! PALM is free software: you can redistribute it and/or modify it under the terms
! of the GNU General Public License as published by the Free Software Foundation,
! either version 3 of the License, or (at your option) any later version.
!
! PALM is distributed in the hope that it will be useful, but WITHOUT ANY
! WARRANTY; without even the implied warranty of MERCHANTABILITY or FITNESS FOR
! A PARTICULAR PURPOSE.  See the GNU General Public License for more details.
!
! You should have received a copy of the GNU General Public License along with
! PALM. If not, see <http://www.gnu.org/licenses/>.
!
! Copyright 1997-2012  Leibniz University Hannover
!--------------------------------------------------------------------------------!
!
! Current revisions:
! -----------------
!
!  
! Former revisions:
! -----------------
! $Id: boundary_conds.f90 1160 2013-05-21 12:06:24Z heinze $
!
! 1159 2013-05-21 11:58:22Z fricke
! Bugfix: Neumann boundary conditions for the velocity components at the
! outflow are in fact radiation boundary conditions using the maximum phase
! velocity that ensures numerical stability (CFL-condition).
! Hence, logical operator use_cmax is now used instead of bc_lr_dirneu/_neudir.
! Bugfix: In case of use_cmax at the outflow, u, v, w are replaced by
! u_p, v_p, w_p  
!
! 1115 2013-03-26 18:16:16Z hoffmann
! boundary conditions of two-moment cloud scheme are restricted to Neumann-
! boundary-conditions
!
! 1113 2013-03-10 02:48:14Z raasch
! GPU-porting
! dummy argument "range" removed
! Bugfix: wrong index in loops of radiation boundary condition
!
! 1053 2012-11-13 17:11:03Z hoffmann
! boundary conditions for the two new prognostic equations (nr, qr) of the 
! two-moment cloud scheme
!
! 1036 2012-10-22 13:43:42Z raasch
! code put under GPL (PALM 3.9)
!
! 996 2012-09-07 10:41:47Z raasch
! little reformatting
!
! 978 2012-08-09 08:28:32Z fricke
! Neumann boudnary conditions are added at the inflow boundary for the SGS-TKE.
! Outflow boundary conditions for the velocity components can be set to Neumann
! conditions or to radiation conditions with a horizontal averaged phase
! velocity. 
!
! 875 2012-04-02 15:35:15Z gryschka
! Bugfix in case of dirichlet inflow bc at the right or north boundary
!
! 767 2011-10-14 06:39:12Z raasch
! ug,vg replaced by u_init,v_init as the Dirichlet top boundary condition
!
! 667 2010-12-23 12:06:00Z suehring/gryschka
! nxl-1, nxr+1, nys-1, nyn+1 replaced by nxlg, nxrg, nysg, nyng
! Removed mirror boundary conditions for u and v at the bottom in case of 
! ibc_uv_b == 0. Instead, dirichelt boundary conditions (u=v=0) are set
! in init_3d_model 
!
! 107 2007-08-17 13:54:45Z raasch
! Boundary conditions for temperature adjusted for coupled runs,
! bugfixes for the radiation boundary conditions at the outflow: radiation
! conditions are used for every substep, phase speeds are calculated for the
! first Runge-Kutta substep only and then reused, several index values changed
!
! 95 2007-06-02 16:48:38Z raasch
! Boundary conditions for salinity added
!
! 75 2007-03-22 09:54:05Z raasch
! The "main" part sets conditions for time level t+dt instead of level t,
! outflow boundary conditions changed from Neumann to radiation condition,
! uxrp, vynp eliminated, moisture renamed humidity
!
! 19 2007-02-23 04:53:48Z raasch
! Boundary conditions for e(nzt), pt(nzt), and q(nzt) removed because these
! gridpoints are now calculated by the prognostic equation,
! Dirichlet and zero gradient condition for pt established at top boundary
!
! RCS Log replace by Id keyword, revision history cleaned up
!
! Revision 1.15  2006/02/23 09:54:55  raasch
! Surface boundary conditions in case of topography: nzb replaced by
! 2d-k-index-arrays (nzb_w_inner, etc.). Conditions for u and v remain
! unchanged (still using nzb) because a non-flat topography must use a
! Prandtl-layer, which don't requires explicit setting of the surface values.
!
! Revision 1.1  1997/09/12 06:21:34  raasch
! Initial revision
!
!
! Description:
! ------------
! Boundary conditions for the prognostic quantities.
! One additional bottom boundary condition is applied for the TKE (=(u*)**2)
! in prandtl_fluxes. The cyclic lateral boundary conditions are implicitly
! handled in routine exchange_horiz. Pressure boundary conditions are
! explicitly set in routines pres, poisfft, poismg and sor.
!------------------------------------------------------------------------------!

    USE arrays_3d
    USE control_parameters
    USE grid_variables
    USE indices
    USE pegrid

    IMPLICIT NONE

    INTEGER ::  i, j, k

    REAL    ::  c_max, denom


!
!-- Bottom boundary 
    IF ( ibc_uv_b == 1 )  THEN
       !$acc kernels present( u_p, v_p )
       u_p(nzb,:,:) = u_p(nzb+1,:,:)
       v_p(nzb,:,:) = v_p(nzb+1,:,:)
       !$acc end kernels
    ENDIF

    !$acc kernels present( nzb_w_inner, w_p )
    DO  i = nxlg, nxrg
       DO  j = nysg, nyng
          w_p(nzb_w_inner(j,i),j,i) = 0.0
       ENDDO
    ENDDO
    !$acc end kernels

!
!-- Top boundary
    IF ( ibc_uv_t == 0 )  THEN
       !$acc kernels present( u_init, u_p, v_init, v_p )
        u_p(nzt+1,:,:) = u_init(nzt+1)
        v_p(nzt+1,:,:) = v_init(nzt+1)
       !$acc end kernels
    ELSE
       !$acc kernels present( u_p, v_p )
        u_p(nzt+1,:,:) = u_p(nzt,:,:)
        v_p(nzt+1,:,:) = v_p(nzt,:,:)
       !$acc end kernels
    ENDIF
    !$acc kernels present( w_p )
    w_p(nzt:nzt+1,:,:) = 0.0  ! nzt is not a prognostic level (but cf. pres)
    !$acc end kernels

!
!-- Temperature at bottom boundary.
!-- In case of coupled runs (ibc_pt_b = 2) the temperature is given by
!-- the sea surface temperature of the coupled ocean model.
    IF ( ibc_pt_b == 0 )  THEN
       !$acc kernels present( nzb_s_inner, pt, pt_p )
       DO  i = nxlg, nxrg
          DO  j = nysg, nyng
             pt_p(nzb_s_inner(j,i),j,i) = pt(nzb_s_inner(j,i),j,i)
          ENDDO
       ENDDO
       !$acc end kernels
    ELSEIF ( ibc_pt_b == 1 )  THEN
       !$acc kernels present( nzb_s_inner, pt_p )
       DO  i = nxlg, nxrg
          DO  j = nysg, nyng
             pt_p(nzb_s_inner(j,i),j,i) = pt_p(nzb_s_inner(j,i)+1,j,i)
          ENDDO
       ENDDO
      !$acc end kernels
    ENDIF

!
!-- Temperature at top boundary
    IF ( ibc_pt_t == 0 )  THEN
       !$acc kernels present( pt, pt_p )
        pt_p(nzt+1,:,:) = pt(nzt+1,:,:)
       !$acc end kernels
    ELSEIF ( ibc_pt_t == 1 )  THEN
       !$acc kernels present( pt_p )
        pt_p(nzt+1,:,:) = pt_p(nzt,:,:)
       !$acc end kernels
    ELSEIF ( ibc_pt_t == 2 )  THEN
       !$acc kernels present( dzu, pt_p )
        pt_p(nzt+1,:,:) = pt_p(nzt,:,:)   + bc_pt_t_val * dzu(nzt+1)
       !$acc end kernels
    ENDIF

!
!-- Boundary conditions for TKE
!-- Generally Neumann conditions with de/dz=0 are assumed
    IF ( .NOT. constant_diffusion )  THEN
       !$acc kernels present( e_p, nzb_s_inner )
       DO  i = nxlg, nxrg
          DO  j = nysg, nyng
             e_p(nzb_s_inner(j,i),j,i) = e_p(nzb_s_inner(j,i)+1,j,i)
          ENDDO
       ENDDO
       e_p(nzt+1,:,:) = e_p(nzt,:,:)
       !$acc end kernels
    ENDIF

!
!-- Boundary conditions for salinity
    IF ( ocean )  THEN
!
!--    Bottom boundary: Neumann condition because salinity flux is always
!--    given
       DO  i = nxlg, nxrg
          DO  j = nysg, nyng
             sa_p(nzb_s_inner(j,i),j,i) = sa_p(nzb_s_inner(j,i)+1,j,i)
          ENDDO
       ENDDO

!
!--    Top boundary: Dirichlet or Neumann
       IF ( ibc_sa_t == 0 )  THEN
           sa_p(nzt+1,:,:) = sa(nzt+1,:,:)
       ELSEIF ( ibc_sa_t == 1 )  THEN
           sa_p(nzt+1,:,:) = sa_p(nzt,:,:)
       ENDIF

    ENDIF

!
!-- Boundary conditions for total water content or scalar,
!-- bottom and top boundary (see also temperature)
    IF ( humidity  .OR.  passive_scalar )  THEN
!
!--    Surface conditions for constant_humidity_flux
       IF ( ibc_q_b == 0 ) THEN
          DO  i = nxlg, nxrg
             DO  j = nysg, nyng
                q_p(nzb_s_inner(j,i),j,i) = q(nzb_s_inner(j,i),j,i)
             ENDDO
          ENDDO
       ELSE
          DO  i = nxlg, nxrg
             DO  j = nysg, nyng
                q_p(nzb_s_inner(j,i),j,i) = q_p(nzb_s_inner(j,i)+1,j,i)
             ENDDO
          ENDDO
       ENDIF
!
!--    Top boundary
       q_p(nzt+1,:,:) = q_p(nzt,:,:)   + bc_q_t_val * dzu(nzt+1)

       IF ( cloud_physics  .AND.  icloud_scheme == 0  .AND.  &
            precipitation )  THEN
!             
!--       Surface conditions rain water (Neumann)
          DO  i = nxlg, nxrg
             DO  j = nysg, nyng
                qr_p(nzb_s_inner(j,i),j,i) = qr_p(nzb_s_inner(j,i)+1,j,i)
                nr_p(nzb_s_inner(j,i),j,i) = nr_p(nzb_s_inner(j,i)+1,j,i)
             ENDDO
          ENDDO
!
!--       Top boundary condition for rain water (Neumann)
          qr_p(nzt+1,:,:) = qr_p(nzt,:,:)
          nr_p(nzt+1,:,:) = nr_p(nzt,:,:)
           
       ENDIF
!
!--    In case of inflow at the south boundary the boundary for v is at nys
!--    and in case of inflow at the left boundary the boundary for u is at nxl.
!--    Since in prognostic_equations (cache optimized version) these levels are
!--    handled as a prognostic level, boundary values have to be restored here.
!--    For the SGS-TKE, Neumann boundary conditions are used at the inflow.
       IF ( inflow_s )  THEN
          v_p(:,nys,:) = v_p(:,nys-1,:)
          IF ( .NOT. constant_diffusion ) e_p(:,nys-1,:) = e_p(:,nys,:)
       ELSEIF ( inflow_n )  THEN
          IF ( .NOT. constant_diffusion ) e_p(:,nyn+1,:) = e_p(:,nyn,:)
       ELSEIF ( inflow_l ) THEN
          u_p(:,:,nxl) = u_p(:,:,nxl-1)
          IF ( .NOT. constant_diffusion ) e_p(:,:,nxl-1) = e_p(:,:,nxl)
       ELSEIF ( inflow_r )  THEN
          IF ( .NOT. constant_diffusion ) e_p(:,:,nxr+1) = e_p(:,:,nxr)
       ENDIF

!
!--    Lateral boundary conditions for scalar quantities at the outflow
       IF ( outflow_s )  THEN
          pt_p(:,nys-1,:)     = pt_p(:,nys,:)
          IF ( .NOT. constant_diffusion     )  e_p(:,nys-1,:) = e_p(:,nys,:)
          IF ( humidity  .OR.  passive_scalar )  THEN
             q_p(:,nys-1,:) = q_p(:,nys,:)
             IF ( cloud_physics  .AND.  icloud_scheme == 0  .AND.  &
                  precipitation)  THEN
                qr_p(:,nys-1,:) = qr_p(:,nys,:)
                nr_p(:,nys-1,:) = nr_p(:,nys,:)
             ENDIF
          ENDIF
       ELSEIF ( outflow_n )  THEN
          pt_p(:,nyn+1,:)     = pt_p(:,nyn,:)
          IF ( .NOT. constant_diffusion     )  e_p(:,nyn+1,:) = e_p(:,nyn,:)
          IF ( humidity  .OR.  passive_scalar )  THEN
             q_p(:,nyn+1,:) = q_p(:,nyn,:)
             IF ( cloud_physics  .AND.  icloud_scheme == 0  .AND.  &
                  precipitation )  THEN
                qr_p(:,nyn+1,:) = qr_p(:,nyn,:)
                nr_p(:,nyn+1,:) = nr_p(:,nyn,:)
             ENDIF
          ENDIF
       ELSEIF ( outflow_l )  THEN
          pt_p(:,:,nxl-1)     = pt_p(:,:,nxl)
          IF ( .NOT. constant_diffusion     )  e_p(:,:,nxl-1) = e_p(:,:,nxl)
          IF ( humidity  .OR.  passive_scalar )  THEN
             q_p(:,:,nxl-1) = q_p(:,:,nxl)
             IF ( cloud_physics  .AND.  icloud_scheme == 0  .AND.  &
                  precipitation )  THEN
                qr_p(:,:,nxl-1) = qr_p(:,:,nxl)
                nr_p(:,:,nxl-1) = nr_p(:,:,nxl)
             ENDIF
          ENDIF
       ELSEIF ( outflow_r )  THEN
          pt_p(:,:,nxr+1)     = pt_p(:,:,nxr)
          IF ( .NOT. constant_diffusion     )  e_p(:,:,nxr+1) = e_p(:,:,nxr)
          IF ( humidity .OR. passive_scalar )  THEN
             q_p(:,:,nxr+1) = q_p(:,:,nxr)
             IF ( cloud_physics  .AND.  icloud_scheme == 0  .AND.  precipitation )  THEN
                qr_p(:,:,nxr+1) = qr_p(:,:,nxr)
                nr_p(:,:,nxr+1) = nr_p(:,:,nxr)
             ENDIF
          ENDIF
       ENDIF

    ENDIF

!
!-- Radiation boundary conditions for the velocities at the respective outflow.
!-- The phase velocity is either assumed to the maximum phase velocity that
!-- ensures numerical stability (CFL-condition) or calculated after
!-- Orlanski(1976) and averaged along the outflow boundary.
    IF ( outflow_s )  THEN

       IF ( use_cmax )  THEN
          u_p(:,-1,:) = u(:,0,:)
          v_p(:,0,:)  = v(:,1,:)
          w_p(:,-1,:) = w(:,0,:)          
       ELSEIF ( .NOT. use_cmax )  THEN

          c_max = dy / dt_3d

          c_u_m_l = 0.0 
          c_v_m_l = 0.0
          c_w_m_l = 0.0

          c_u_m = 0.0 
          c_v_m = 0.0
          c_w_m = 0.0

!
!--       Calculate the phase speeds for u, v, and w, first local and then
!--       average along the outflow boundary.
          DO  k = nzb+1, nzt+1
             DO  i = nxl, nxr

                denom = u_m_s(k,0,i) - u_m_s(k,1,i)

                IF ( denom /= 0.0 )  THEN
                   c_u(k,i) = -c_max * ( u(k,0,i) - u_m_s(k,0,i) ) / ( denom * tsc(2) )
                   IF ( c_u(k,i) < 0.0 )  THEN
                      c_u(k,i) = 0.0
                   ELSEIF ( c_u(k,i) > c_max )  THEN
                      c_u(k,i) = c_max
                   ENDIF
                ELSE
                   c_u(k,i) = c_max
                ENDIF

                denom = v_m_s(k,1,i) - v_m_s(k,2,i)

                IF ( denom /= 0.0 )  THEN
                   c_v(k,i) = -c_max * ( v(k,1,i) - v_m_s(k,1,i) ) / ( denom * tsc(2) )
                   IF ( c_v(k,i) < 0.0 )  THEN
                      c_v(k,i) = 0.0
                   ELSEIF ( c_v(k,i) > c_max )  THEN
                      c_v(k,i) = c_max
                   ENDIF
                ELSE
                   c_v(k,i) = c_max
                ENDIF

                denom = w_m_s(k,0,i) - w_m_s(k,1,i)

                IF ( denom /= 0.0 )  THEN
                   c_w(k,i) = -c_max * ( w(k,0,i) - w_m_s(k,0,i) ) / ( denom * tsc(2) )
                   IF ( c_w(k,i) < 0.0 )  THEN
                      c_w(k,i) = 0.0
                   ELSEIF ( c_w(k,i) > c_max )  THEN
                      c_w(k,i) = c_max
                   ENDIF
                ELSE
                   c_w(k,i) = c_max
                ENDIF

                c_u_m_l(k) = c_u_m_l(k) + c_u(k,i)
                c_v_m_l(k) = c_v_m_l(k) + c_v(k,i)
                c_w_m_l(k) = c_w_m_l(k) + c_w(k,i)

             ENDDO
          ENDDO

#if defined( __parallel )   
          IF ( collective_wait )  CALL MPI_BARRIER( comm1dx, ierr )
          CALL MPI_ALLREDUCE( c_u_m_l(nzb+1), c_u_m(nzb+1), nzt-nzb, MPI_REAL, &
                              MPI_SUM, comm1dx, ierr )   
          IF ( collective_wait )  CALL MPI_BARRIER( comm1dx, ierr )
          CALL MPI_ALLREDUCE( c_v_m_l(nzb+1), c_v_m(nzb+1), nzt-nzb, MPI_REAL, &
                              MPI_SUM, comm1dx, ierr )  
          IF ( collective_wait )  CALL MPI_BARRIER( comm1dx, ierr )
          CALL MPI_ALLREDUCE( c_w_m_l(nzb+1), c_w_m(nzb+1), nzt-nzb, MPI_REAL, &
                              MPI_SUM, comm1dx, ierr )  
#else
          c_u_m = c_u_m_l
          c_v_m = c_v_m_l
          c_w_m = c_w_m_l
#endif

          c_u_m = c_u_m / (nx+1)
          c_v_m = c_v_m / (nx+1)
          c_w_m = c_w_m / (nx+1)

!
!--       Save old timelevels for the next timestep
          IF ( intermediate_timestep_count == 1 )  THEN
             u_m_s(:,:,:) = u(:,0:1,:)
             v_m_s(:,:,:) = v(:,1:2,:)
             w_m_s(:,:,:) = w(:,0:1,:)
          ENDIF

!
!--       Calculate the new velocities
          DO  k = nzb+1, nzt+1
             DO  i = nxlg, nxrg
                u_p(k,-1,i) = u(k,-1,i) - dt_3d * tsc(2) * c_u_m(k) *          &
                                       ( u(k,-1,i) - u(k,0,i) ) * ddy

                v_p(k,0,i)  = v(k,0,i)  - dt_3d * tsc(2) * c_v_m(k) *          &
                                       ( v(k,0,i) - v(k,1,i) ) * ddy

                w_p(k,-1,i) = w(k,-1,i) - dt_3d * tsc(2) * c_w_m(k) *          &
                                       ( w(k,-1,i) - w(k,0,i) ) * ddy
             ENDDO
          ENDDO

!
!--       Bottom boundary at the outflow
          IF ( ibc_uv_b == 0 )  THEN
             u_p(nzb,-1,:) = 0.0 
             v_p(nzb,0,:)  = 0.0  
          ELSE                    
             u_p(nzb,-1,:) =  u_p(nzb+1,-1,:)
             v_p(nzb,0,:)  =  v_p(nzb+1,0,:)
          ENDIF
          w_p(nzb,-1,:) = 0.0

!
!--       Top boundary at the outflow
          IF ( ibc_uv_t == 0 )  THEN
             u_p(nzt+1,-1,:) = u_init(nzt+1)
             v_p(nzt+1,0,:)  = v_init(nzt+1)
          ELSE
             u_p(nzt+1,-1,:) = u(nzt,-1,:)
             v_p(nzt+1,0,:)  = v(nzt,0,:)
          ENDIF
          w_p(nzt:nzt+1,-1,:) = 0.0

       ENDIF

    ENDIF

    IF ( outflow_n )  THEN

       IF ( use_cmax )  THEN
          u_p(:,ny+1,:) = u(:,ny,:)
          v_p(:,ny+1,:) = v(:,ny,:)
          w_p(:,ny+1,:) = w(:,ny,:)          
       ELSEIF ( .NOT. use_cmax )  THEN

          c_max = dy / dt_3d

          c_u_m_l = 0.0 
          c_v_m_l = 0.0
          c_w_m_l = 0.0

          c_u_m = 0.0 
          c_v_m = 0.0
          c_w_m = 0.0

!
!--       Calculate the phase speeds for u, v, and w, first local and then
!--       average along the outflow boundary.
          DO  k = nzb+1, nzt+1
             DO  i = nxl, nxr

                denom = u_m_n(k,ny,i) - u_m_n(k,ny-1,i)

                IF ( denom /= 0.0 )  THEN
                   c_u(k,i) = -c_max * ( u(k,ny,i) - u_m_n(k,ny,i) ) / ( denom * tsc(2) )
                   IF ( c_u(k,i) < 0.0 )  THEN
                      c_u(k,i) = 0.0
                   ELSEIF ( c_u(k,i) > c_max )  THEN
                      c_u(k,i) = c_max
                   ENDIF
                ELSE
                   c_u(k,i) = c_max
                ENDIF

                denom = v_m_n(k,ny,i) - v_m_n(k,ny-1,i)

                IF ( denom /= 0.0 )  THEN
                   c_v(k,i) = -c_max * ( v(k,ny,i) - v_m_n(k,ny,i) ) / ( denom * tsc(2) )
                   IF ( c_v(k,i) < 0.0 )  THEN
                      c_v(k,i) = 0.0
                   ELSEIF ( c_v(k,i) > c_max )  THEN
                      c_v(k,i) = c_max
                   ENDIF
                ELSE
                   c_v(k,i) = c_max
                ENDIF

                denom = w_m_n(k,ny,i) - w_m_n(k,ny-1,i)

                IF ( denom /= 0.0 )  THEN
                   c_w(k,i) = -c_max * ( w(k,ny,i) - w_m_n(k,ny,i) ) / ( denom * tsc(2) )
                   IF ( c_w(k,i) < 0.0 )  THEN
                      c_w(k,i) = 0.0
                   ELSEIF ( c_w(k,i) > c_max )  THEN
                      c_w(k,i) = c_max
                   ENDIF
                ELSE
                   c_w(k,i) = c_max
                ENDIF

                c_u_m_l(k) = c_u_m_l(k) + c_u(k,i)
                c_v_m_l(k) = c_v_m_l(k) + c_v(k,i)
                c_w_m_l(k) = c_w_m_l(k) + c_w(k,i)

             ENDDO
          ENDDO

#if defined( __parallel )   
          IF ( collective_wait )  CALL MPI_BARRIER( comm1dx, ierr )
          CALL MPI_ALLREDUCE( c_u_m_l(nzb+1), c_u_m(nzb+1), nzt-nzb, MPI_REAL, &
                              MPI_SUM, comm1dx, ierr )   
          IF ( collective_wait )  CALL MPI_BARRIER( comm1dx, ierr )
          CALL MPI_ALLREDUCE( c_v_m_l(nzb+1), c_v_m(nzb+1), nzt-nzb, MPI_REAL, &
                              MPI_SUM, comm1dx, ierr )  
          IF ( collective_wait )  CALL MPI_BARRIER( comm1dx, ierr )
          CALL MPI_ALLREDUCE( c_w_m_l(nzb+1), c_w_m(nzb+1), nzt-nzb, MPI_REAL, &
                              MPI_SUM, comm1dx, ierr )  
#else
          c_u_m = c_u_m_l
          c_v_m = c_v_m_l
          c_w_m = c_w_m_l
#endif

          c_u_m = c_u_m / (nx+1)
          c_v_m = c_v_m / (nx+1)
          c_w_m = c_w_m / (nx+1)

!
!--       Save old timelevels for the next timestep
          IF ( intermediate_timestep_count == 1 )  THEN
                u_m_n(:,:,:) = u(:,ny-1:ny,:)
                v_m_n(:,:,:) = v(:,ny-1:ny,:)
                w_m_n(:,:,:) = w(:,ny-1:ny,:)
          ENDIF

!
!--       Calculate the new velocities
          DO  k = nzb+1, nzt+1
             DO  i = nxlg, nxrg
                u_p(k,ny+1,i) = u(k,ny+1,i) - dt_3d * tsc(2) * c_u_m(k) *      &
                                       ( u(k,ny+1,i) - u(k,ny,i) ) * ddy

                v_p(k,ny+1,i) = v(k,ny+1,i)  - dt_3d * tsc(2) * c_v_m(k) *     &
                                       ( v(k,ny+1,i) - v(k,ny,i) ) * ddy

                w_p(k,ny+1,i) = w(k,ny+1,i) - dt_3d * tsc(2) * c_w_m(k) *      &
                                       ( w(k,ny+1,i) - w(k,ny,i) ) * ddy
             ENDDO
          ENDDO

!
!--       Bottom boundary at the outflow
          IF ( ibc_uv_b == 0 )  THEN
             u_p(nzb,ny+1,:) = 0.0 
             v_p(nzb,ny+1,:) = 0.0   
          ELSE                    
             u_p(nzb,ny+1,:) =  u_p(nzb+1,ny+1,:)
             v_p(nzb,ny+1,:) =  v_p(nzb+1,ny+1,:)
          ENDIF
          w_p(nzb,ny+1,:) = 0.0

!
!--       Top boundary at the outflow
          IF ( ibc_uv_t == 0 )  THEN
             u_p(nzt+1,ny+1,:) = u_init(nzt+1)
             v_p(nzt+1,ny+1,:) = v_init(nzt+1)
          ELSE
             u_p(nzt+1,ny+1,:) = u_p(nzt,nyn+1,:)
             v_p(nzt+1,ny+1,:) = v_p(nzt,nyn+1,:)
          ENDIF
          w_p(nzt:nzt+1,ny+1,:) = 0.0

       ENDIF

    ENDIF

    IF ( outflow_l )  THEN

       IF ( use_cmax )  THEN
          u_p(:,:,-1) = u(:,:,0)
          v_p(:,:,0)  = v(:,:,1)
          w_p(:,:,-1) = w(:,:,0)          
       ELSEIF ( .NOT. use_cmax )  THEN

          c_max = dx / dt_3d

          c_u_m_l = 0.0 
          c_v_m_l = 0.0
          c_w_m_l = 0.0

          c_u_m = 0.0 
          c_v_m = 0.0
          c_w_m = 0.0

!
!--       Calculate the phase speeds for u, v, and w, first local and then
!--       average along the outflow boundary.
          DO  k = nzb+1, nzt+1
             DO  j = nys, nyn

                denom = u_m_l(k,j,1) - u_m_l(k,j,2)

                IF ( denom /= 0.0 )  THEN
                   c_u(k,j) = -c_max * ( u(k,j,1) - u_m_l(k,j,1) ) / ( denom * tsc(2) )
                   IF ( c_u(k,j) < 0.0 )  THEN
                      c_u(k,j) = 0.0
                   ELSEIF ( c_u(k,j) > c_max )  THEN
                      c_u(k,j) = c_max
                   ENDIF
                ELSE
                   c_u(k,j) = c_max
                ENDIF

                denom = v_m_l(k,j,0) - v_m_l(k,j,1)

                IF ( denom /= 0.0 )  THEN
                   c_v(k,j) = -c_max * ( v(k,j,0) - v_m_l(k,j,0) ) / ( denom * tsc(2) )
                   IF ( c_v(k,j) < 0.0 )  THEN
                      c_v(k,j) = 0.0
                   ELSEIF ( c_v(k,j) > c_max )  THEN
                      c_v(k,j) = c_max
                   ENDIF
                ELSE
                   c_v(k,j) = c_max
                ENDIF

                denom = w_m_l(k,j,0) - w_m_l(k,j,1)

                IF ( denom /= 0.0 )  THEN
                   c_w(k,j) = -c_max * ( w(k,j,0) - w_m_l(k,j,0) ) / ( denom * tsc(2) )
                   IF ( c_w(k,j) < 0.0 )  THEN
                      c_w(k,j) = 0.0
                   ELSEIF ( c_w(k,j) > c_max )  THEN
                      c_w(k,j) = c_max
                   ENDIF
                ELSE
                   c_w(k,j) = c_max
                ENDIF

                c_u_m_l(k) = c_u_m_l(k) + c_u(k,j)
                c_v_m_l(k) = c_v_m_l(k) + c_v(k,j)
                c_w_m_l(k) = c_w_m_l(k) + c_w(k,j)

             ENDDO
          ENDDO

#if defined( __parallel )   
          IF ( collective_wait )  CALL MPI_BARRIER( comm1dy, ierr )
          CALL MPI_ALLREDUCE( c_u_m_l(nzb+1), c_u_m(nzb+1), nzt-nzb, MPI_REAL, &
                              MPI_SUM, comm1dy, ierr )   
          IF ( collective_wait )  CALL MPI_BARRIER( comm1dy, ierr )
          CALL MPI_ALLREDUCE( c_v_m_l(nzb+1), c_v_m(nzb+1), nzt-nzb, MPI_REAL, &
                              MPI_SUM, comm1dy, ierr )  
          IF ( collective_wait )  CALL MPI_BARRIER( comm1dy, ierr )
          CALL MPI_ALLREDUCE( c_w_m_l(nzb+1), c_w_m(nzb+1), nzt-nzb, MPI_REAL, &
                              MPI_SUM, comm1dy, ierr )  
#else
          c_u_m = c_u_m_l
          c_v_m = c_v_m_l
          c_w_m = c_w_m_l
#endif

          c_u_m = c_u_m / (ny+1)
          c_v_m = c_v_m / (ny+1)
          c_w_m = c_w_m / (ny+1)

!
!--       Save old timelevels for the next timestep
          IF ( intermediate_timestep_count == 1 )  THEN
                u_m_l(:,:,:) = u(:,:,1:2)
                v_m_l(:,:,:) = v(:,:,0:1)
                w_m_l(:,:,:) = w(:,:,0:1)
          ENDIF

!
!--       Calculate the new velocities
          DO  k = nzb+1, nzt+1
             DO  j = nysg, nyng
                u_p(k,j,0) = u(k,j,0) - dt_3d * tsc(2) * c_u_m(k) *            &
                                       ( u(k,j,0) - u(k,j,1) ) * ddx

                v_p(k,j,-1) = v(k,j,-1) - dt_3d * tsc(2) * c_v_m(k) *          &
                                       ( v(k,j,-1) - v(k,j,0) ) * ddx

                w_p(k,j,-1) = w(k,j,-1) - dt_3d * tsc(2) * c_w_m(k) *          &
                                       ( w(k,j,-1) - w(k,j,0) ) * ddx
             ENDDO
          ENDDO

!
!--       Bottom boundary at the outflow
          IF ( ibc_uv_b == 0 )  THEN
             u_p(nzb,:,0)  = 0.0 
             v_p(nzb,:,-1) = 0.0
          ELSE                    
             u_p(nzb,:,0)  =  u_p(nzb+1,:,0)
             v_p(nzb,:,-1) =  v_p(nzb+1,:,-1)
          ENDIF
          w_p(nzb,:,-1) = 0.0

!
!--       Top boundary at the outflow
          IF ( ibc_uv_t == 0 )  THEN
             u_p(nzt+1,:,-1) = u_init(nzt+1)
             v_p(nzt+1,:,-1) = v_init(nzt+1)
          ELSE
             u_p(nzt+1,:,-1) = u_p(nzt,:,-1)
             v_p(nzt+1,:,-1) = v_p(nzt,:,-1)
          ENDIF
          w_p(nzt:nzt+1,:,-1) = 0.0

       ENDIF

    ENDIF

    IF ( outflow_r )  THEN

       IF ( use_cmax )  THEN
          u_p(:,:,nx+1) = u(:,:,nx)
          v_p(:,:,nx+1) = v(:,:,nx)
          w_p(:,:,nx+1) = w(:,:,nx)          
       ELSEIF ( .NOT. use_cmax )  THEN

          c_max = dx / dt_3d

          c_u_m_l = 0.0 
          c_v_m_l = 0.0
          c_w_m_l = 0.0

          c_u_m = 0.0 
          c_v_m = 0.0
          c_w_m = 0.0

!
!--       Calculate the phase speeds for u, v, and w, first local and then
!--       average along the outflow boundary.
          DO  k = nzb+1, nzt+1
             DO  j = nys, nyn

                denom = u_m_r(k,j,nx) - u_m_r(k,j,nx-1)

                IF ( denom /= 0.0 )  THEN
                   c_u(k,j) = -c_max * ( u(k,j,nx) - u_m_r(k,j,nx) ) / ( denom * tsc(2) )
                   IF ( c_u(k,j) < 0.0 )  THEN
                      c_u(k,j) = 0.0
                   ELSEIF ( c_u(k,j) > c_max )  THEN
                      c_u(k,j) = c_max
                   ENDIF
                ELSE
                   c_u(k,j) = c_max
                ENDIF

                denom = v_m_r(k,j,nx) - v_m_r(k,j,nx-1)

                IF ( denom /= 0.0 )  THEN
                   c_v(k,j) = -c_max * ( v(k,j,nx) - v_m_r(k,j,nx) ) / ( denom * tsc(2) )
                   IF ( c_v(k,j) < 0.0 )  THEN
                      c_v(k,j) = 0.0
                   ELSEIF ( c_v(k,j) > c_max )  THEN
                      c_v(k,j) = c_max
                   ENDIF
                ELSE
                   c_v(k,j) = c_max
                ENDIF

                denom = w_m_r(k,j,nx) - w_m_r(k,j,nx-1)

                IF ( denom /= 0.0 )  THEN
                   c_w(k,j) = -c_max * ( w(k,j,nx) - w_m_r(k,j,nx) ) / ( denom * tsc(2) )
                   IF ( c_w(k,j) < 0.0 )  THEN
                      c_w(k,j) = 0.0
                   ELSEIF ( c_w(k,j) > c_max )  THEN
                      c_w(k,j) = c_max
                   ENDIF
                ELSE
                   c_w(k,j) = c_max
                ENDIF

                c_u_m_l(k) = c_u_m_l(k) + c_u(k,j)
                c_v_m_l(k) = c_v_m_l(k) + c_v(k,j)
                c_w_m_l(k) = c_w_m_l(k) + c_w(k,j)

             ENDDO
          ENDDO

#if defined( __parallel )   
          IF ( collective_wait )  CALL MPI_BARRIER( comm1dy, ierr )
          CALL MPI_ALLREDUCE( c_u_m_l(nzb+1), c_u_m(nzb+1), nzt-nzb, MPI_REAL, &
                              MPI_SUM, comm1dy, ierr )   
          IF ( collective_wait )  CALL MPI_BARRIER( comm1dy, ierr )
          CALL MPI_ALLREDUCE( c_v_m_l(nzb+1), c_v_m(nzb+1), nzt-nzb, MPI_REAL, &
                              MPI_SUM, comm1dy, ierr )  
          IF ( collective_wait )  CALL MPI_BARRIER( comm1dy, ierr )
          CALL MPI_ALLREDUCE( c_w_m_l(nzb+1), c_w_m(nzb+1), nzt-nzb, MPI_REAL, &
                              MPI_SUM, comm1dy, ierr )  
#else
          c_u_m = c_u_m_l
          c_v_m = c_v_m_l
          c_w_m = c_w_m_l
#endif

          c_u_m = c_u_m / (ny+1)
          c_v_m = c_v_m / (ny+1)
          c_w_m = c_w_m / (ny+1)

!
!--       Save old timelevels for the next timestep
          IF ( intermediate_timestep_count == 1 )  THEN
                u_m_r(:,:,:) = u(:,:,nx-1:nx)
                v_m_r(:,:,:) = v(:,:,nx-1:nx)
                w_m_r(:,:,:) = w(:,:,nx-1:nx)
          ENDIF

!
!--       Calculate the new velocities
          DO  k = nzb+1, nzt+1
             DO  j = nysg, nyng
                u_p(k,j,nx+1) = u(k,j,nx+1) - dt_3d * tsc(2) * c_u_m(k) *      &
                                       ( u(k,j,nx+1) - u(k,j,nx) ) * ddx

                v_p(k,j,nx+1) = v(k,j,nx+1) - dt_3d * tsc(2) * c_v_m(k) *      &
                                       ( v(k,j,nx+1) - v(k,j,nx) ) * ddx

                w_p(k,j,nx+1) = w(k,j,nx+1) - dt_3d * tsc(2) * c_w_m(k) *      &
                                       ( w(k,j,nx+1) - w(k,j,nx) ) * ddx
             ENDDO
          ENDDO

!
!--       Bottom boundary at the outflow
          IF ( ibc_uv_b == 0 )  THEN
             u_p(nzb,:,nx+1) = 0.0
             v_p(nzb,:,nx+1) = 0.0 
          ELSE                    
             u_p(nzb,:,nx+1) =  u_p(nzb+1,:,nx+1)
             v_p(nzb,:,nx+1) =  v_p(nzb+1,:,nx+1)
          ENDIF
          w_p(nzb,:,nx+1) = 0.0

!
!--       Top boundary at the outflow
          IF ( ibc_uv_t == 0 )  THEN
             u_p(nzt+1,:,nx+1) = u_init(nzt+1)
             v_p(nzt+1,:,nx+1) = v_init(nzt+1)
          ELSE
             u_p(nzt+1,:,nx+1) = u_p(nzt,:,nx+1)
             v_p(nzt+1,:,nx+1) = v_p(nzt,:,nx+1)
          ENDIF
          w(nzt:nzt+1,:,nx+1) = 0.0

       ENDIF

    ENDIF

 END SUBROUTINE boundary_conds